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Under the condition (formula presented) one can consider the system (28) with the energy fluxes given by Eqs. (29) and (13) as a simplified system with constant coefficients. The general solution for such a system is a linear combination of the fundamental solutions (formula presented) with the roots, determined from the third-order characteristic equation. The coefficients in such linear form are determined from the boundary conditions in Eq. (32) and the normalization condition in Eq. (17)
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